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PHY 752 Solid State Physics Reading: Chapter 4 in GGGPP
11-11:50 AM MWF Olin 107 Plan for Lecture 13: Reading: Chapter 4 in GGGPP Approximations to the many electron problem --Density functional theory General theorem Practical calculation scheme Some results 9/23/2015 PHY 752 Fall Lecture 13
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9/23/2015 PHY 752 Fall Lecture 13
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Density functional theory
Describes the relationship between the many electron problem and independent electron treatments. Proof of theorem Estimates of F[n]. 9/23/2015 PHY 752 Fall Lecture 13
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Density functional theory -- continued
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Hohenberg and Kohn: formal proof of basic theorem
Kinetic energy External potential Coulomb interaction 9/23/2015 PHY 752 Fall Lecture 13
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Theorem: The density n(r) of the ground state of the system is a unique functional of the external potential v(r). Proof: Consider two Hamiltonians H and H’ differing only by external potentials v and v’. 9/23/2015 PHY 752 Fall Lecture 13
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We can also show: 9/23/2015 PHY 752 Fall Lecture 13
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The theorem implies that the ground state energy E can be considered as a functional of the density n(r) Thus, the determination of the ground state energy E is transformed into a minimization of the functional with respect to the density n(r), transforming a many particle minimization into a single particle minimization. In practice, the functional form of F[n] is not known, but if it were, we could use optimization methods to determine the ground state energy Ev[n]. 9/23/2015 PHY 752 Fall Lecture 13
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Kohn-Sham scheme to find ground state energy Ev[n]
Assume that the electron density can be expressed in terms of N independent electron orbitals For a given external potential vext(r) the ground state energy is given by E EH[n]= 9/23/2015 PHY 752 Fall Lecture 13
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Kohn-Sham equations where 9/23/2015 PHY 752 Fall Lecture 13
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Estimate of the exchange-correlation contribution
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Digression on spatially varying electron density
j k l 2/13/2015 PHY 752 Spring Lecture 13
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Correlation functionals Local density approximation (LDA)
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Interpolation function for LDA: Ec[n]=
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More complicated exchange-correlation functionals
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Some details of the Generalized Gradient Approximation
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Summary: Kohn-Sham formulation of density functional theory
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Self-consistent solution
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Kohn-Sham formulation of density functional theory
Results of self-consistent calculations Some remaining issues Theory for Eexc[n] still underdevelopment This formalism does not access excited states Strongly correlated electron systems are not well approximated 2/13/2015 PHY 752 Spring Lecture 13
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Comparison of LDA and GGA binding energy curves
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LDA vs GGA performance wrt normal modes of vibration
A: B. N. Mavrin et al, J. Exp. Theor. Phys. 96,53 (2003); B: F. Harbach and F. Fischer, Phys. Status Solidi B 66, 237 (1974) – room temp. C: Ref. B at liquid nitrogen temp.; D: L. Popović et al, J. Raman Spectrosc. 34,77 (2003). 2/13/2015 PHY 752 Spring Lecture 13
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